We present an active physical implementation of the recently introduced plasmon injection loss compensation scheme for Pendry's non-ideal negative index flat lens in the presence of realistic material losses and signal-dependent noise. In this active implementation, we propose to use a physically convolved external auxiliary source for signal amplification and suppression of the noise in the imaging system. In comparison with the previous passive implementations of the plasmon injection scheme for sub-diffraction limited imaging, where an inverse filter post-processing is used, the active implementation proposed here allows for deeper subwavelength imaging far beyond the passive post-processing scheme by extending the loss compensation to even higher spatial frequencies.Although this form of passive inverse filter provides compensation for absorption losses, it is also prone to noise amplification [56]. This is illustrated in figure 1 which shows an object with three Gaussian features separated by λ o /4, where λ o is the free space wavelength. Noise is prominent in the Fourier spectra beyond ky ko = 2.5 as seen in figure 2. However, the compensated image is still reasonably well resolved. Consider now the object shown in figure 3, which has four Gaussians separated by λ o /4. The Fourier spectra of the raw image, shown in figure 4, demonstrates how the feature at